• E2M - 전기 전자와 첨단 소재
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• 제7권2호
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• pp.145-151
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• 1994

The multi-dielectric layer SiOz/Si3N4/SiO2(ONO) is used to scale down the memory device. In this paper, the change of composition in ONO layer due to the process condition and the conduction mechanism are observed. The composition of the oxide film grown through the oxidation of nitride film is analyzed using auger electron spectroscopy(AES). AES results show that oxygen concentration increases at the interface between oxide and nitride layers as the thickness -of the top oxide layer increases. Results of I-V measurement show that the insulating properties improve as the thickness of the top oxide layer increases. But when the thickness of the nitride layer decreases below 63.angs, insulating peoperties of film 28.angs. of top oxide and film 35.angs. turn over showing that insulating property of film 28.angs. of top oxide is better than that of film 35.angs. of top oxide. This phenomenon of turn over is thought as the result of generation of surface state due to oxygen flow into nitride during oxidation process. As the thickness of the top oxide and nitride increases, the electrical breakdown field increases, but when the thickness of top oxide reaches 35.angs, the same phenomenon of turn over occurs. Optimum film thickness for scaled multi-layer dielectric of memory device SONOS is estimated to be 63.angs. of nitride layer and 28.angs. of top oxide layer. In this case, maximum electrical breakdown field and leakage current are 18.5[MV/cm] and $8{\times}{10^-12}$[A], respectively.

• 한국진공학회지
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• 제5권4호
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• pp.327-332
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• 1996

Tungsten(W) polycide gate 구조에서 $WSi_x$의 두께가 증가하면 열처리 공정 후 Gate oxide의 두께가 증가하며, 전기적 신뢰도가 열화 되는 현상이 발생한다. 이러한 특성 열화를 일으키는 지배적인 요인은 $WSi_x$ 증착 공정 중 유입되어 후속 열 공정에 의하여 gate oxide로 환산되는 fluorine인 것으로 밝혀졌다. 이러한 현상을 규명하기 위하여 fluorine ion implantation된 poly Si과의 특성을 비교하였으며, SIMS 및 단면 TEM을 이용한 미세 구조 연구를 실시하였다. 그러나 $WSi_x$의 두께가 600$\AA$ 이상부터는이러한 특성 열화가 포화되는 현상이 관찰되었다. 600$\AA$ 이상의 $WSi_x$ 두께에서는 미세 구조가 표면이 거칠고, porous한 phase로 구성된 상부 구조와 비교적 dense하고, 매끈한 계면 상태를 갖는 하부 구조로 이루어졌으며, porous한 표면 부위는 후속 열공정 중 oxygen-rich한 phase로 변하여 fluorine을 포획하여 oxide로의 확산을 억제하여 특성 열화가 포화되는 것으로 해석되었다.

• 한국정보통신학회논문지
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• 제20권4호
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• pp.799-804
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• 2016

본 논문에서는 비대칭 이중게이트 MOSFET의 상하단 게이트 산화막 두께에 대한 드레인 유도 장벽 감소 현상을 분석하기 위하여 전위장벽에 영향을 미치는 드레인전압에 따른 문턱전압의 변화를 관찰할 것이다. 비대칭 이중게이트 MOSFET는 상단과 하단의 게이트 산화막 두께를 다르게 제작할 수 있는 특징이 있다. 상단과 하단의 게이트 산화막 두께 변화에 따른 드레인 유도 장벽 감소 현상에 대하여 포아송방정식을 이용하여 분석하였다. 결과적으로 드레인 유도 장벽 감소 현상은 상하단 게이트 산화막 두께에 따라 큰 변화를 나타냈다. 상단과 하단 게이트 산화막 두께가 작을수록 드레인 유도 장벽은 선형적으로 감소하였다. 채널길이에 대한 드레인 유도 장벽 감소 값은 비선형적인 관계가 있었다. 고농도 채널도핑의 경우 상단 산화막 두께가 하단 산화막 두께보다 드레인 유도 장벽 감소에 더 큰 영향을 미치고 있었다.

• 한국방사성폐기물학회:학술대회논문집
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• 한국방사성폐기물학회 2005년도 Proceedings of The 6th korea-china joint workshop on nuclear waste management
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• pp.39-50
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• 2005

Electrolytic reduction of uranium oxide to uranium metal was studied in a $LiCl-Li_{2}O$ molten salt system. The reduction mechanism of the uranium oxide to a uranium metal has been studied by means of a cyclic voltammetry. Effects of the layer thickness of the uranium oxide and the thickness of the MgO on the overpotential of the cathode and the anode were investigated by means of a chronopotentiometry. From the cyclic voltamograms, the decomposition potentials of the metal oxides are the determining factors for the mechanism of the reduction of the uranium oxide in a $LiCl-3\;wt{\%} Li_{2}O$ molten salt and the two mechanisms of the electrolytic reduction were considered with regards to the applied cathode potential. In the chronopotentiograms, the exchange current and the transfer coefficient based on the Tafel behavior were obtained with regard to the layer thickness of the uranium oxide which is loaded into the porous MgO membrane and the thickness of the porous MgO membrane. The maximum allowable currents for the changes of the layer thickness of the uranium oxide and the thickness of the MgO membrane were also obtained from the limiting potential which is the decomposition potential of LiCl.

• 한국재료학회:학술대회논문집
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• 한국재료학회 2003년도 추계학술발표강연 및 논문개요집
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• pp.176-176
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• 2003

The effects of oxide thickness and gate length of MgO/GaN metal oxide semiconductor field effect transistors (MOSFETs) on I-V, threshold voltage and breakdown voltage characteristics were examined using a drift-diffusion model. The saturation drain current scales in an inverse logarithmic fashion with MgO thickness and is < 10$^{-3}$ A.${\mu}{\textrm}{m}$$^{-1}$ for 0.5 ${\mu}{\textrm}{m}$ gate length devices with oxide thickness > 600 $\AA$ or for all 1 ${\mu}{\textrm}{m}$ gate length MOSFETs with oxide thickness in the range of >200 $\AA$. Gate breakdown voltage is > 100 V for gate length >0.5 ${\mu}{\textrm}{m}$ and MgO thickness > 600 $\AA$. The threshold voltage scales linearly with oxide thickness and is < 2 V for oxide thickness < 800 $\AA$ and gate lengths < 0.6 ${\mu}{\textrm}{m}$. The GaN MOSFET shows excellent potential for elevated temperature, high speed applications.

• E2M - 전기 전자와 첨단 소재
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• 제9권5호
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• pp.476-482
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• 1996

The multi-dielectric layer SiO$_{2}$/Si$_{3}$N$_{4}$/SiO$_{2}$(ONO) is used to improve electrical capacitance and to scale down the memory device. In this paper, improvement of the capacitance by reducing the bottom oxide thickness in the nitride deposition with load lock(L/L) vacuum system is studied. Bottom oxide thickness under the nitride layer is measured by ellipsometer both in L/L and non-L/L systems. Both results are in the range of 3-10.angs. and 10-15.angs., respectively, independent of the nitride and top oxide thickness. Effective thickness and cell capacitance for SONOS capacitor are in the range of 50-52.angs. and 35-37fF respectively in the case of nitride 70.angs. in L/L vacuum system. Compared with non-L/L system, the bottom oxide thickness in the case of L/L system decreases while cell capacitance increases about 4 fF. The results obtained in this study are also applicable to ONO scaling in the thin bottom oxide region of memory stacked capacitor.

• 한국정보통신학회:학술대회논문집
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• 한국정보통신학회 2013년도 추계학술대회
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• pp.698-701
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• 2013

비대칭 이중게이트(double gate; DG) MOSFET의 문턱전압이하 스윙의 게이트 산화막 두께에 대한 변화를 고찰하였으며 이를 위하여 포아송방정식의 해석학적 전위분포를 구하였다. 비대칭 DGMOSFET 소자는 대칭적 구조를 갖는 DGMOSFET와 달리 4단자 소자로서 상단과 하단의 게이트 산화막 두께 및 인가전압을 달리 설정할 수 있다. 포아송방정식을 풀 때 전하분포함수에 가우시안 함수를 적용함으로써 보다 실험값에 가깝게 해석하였다. 비대칭 DGMOSFET의 문턱전압 이하 스윙을 상 하단 게이트 산화막 두께 변화에 따라 관찰한 결과, 게이트 산화막 두께에 따라 문턱전압이하 스윙은 크게 변화하는 것을 알 수 있었다. 특히 상 하단 게이트 산화막 두께가 증가할 때 문턱전압이하 스윙 값도 증가하였으며 상단 게이트 산화막 두께의 변화가 문턱전압이하 스윙 값에 더욱 큰 영향을 미치고 있다는 것을 알 수 있었다.

• 한국표면공학회지
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• 제33권4호
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• pp.217-221
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• 2000

The gate oxide thickness is becoming thinner and thinner in order to speed up the semiconductor CMOS devices. We have investigated very thin$ SiO_2$ gate oxide layers and found anomaly between the thickness determined with capacitance measurement and these obtained with cross-sectional high resolution transmission electron microscopy. The thicknesses difference of the two becomes important for the thickness of the oxide below 5nm. We propose that the variation of dielectric constant in thin oxide films cause the anomaly. We modeled the behavior as (equation omitted) and determined $\varepsilon_{bulk}$=3.9 and $\varepsilon_{int}$=-4.0. We predict that optimum $SiO_2$ gate oxide thickness may be $20\AA$ due to negative contribution of the interface dielectric constant. These new results have very important implication for designing the CMOS devices.s.

• Corrosion Science and Technology
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• 제9권1호
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• pp.8-11
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• 2010

During PEO (plasma-electrolytic-oxidation) treatment of titanium, the relationship between the thickness of oxide film and the measured electrical information was investigated. A simple real time monitoring method based on the electrical information being gathered during PEO treatment is proposed. The proposed method utilizes the current flowing from a high frequency voltage source to calculate the resistance of an oxide film, which is converted into the thickness of an oxide film. This monitoring method can be implemented in PEO system in which an oxide film is grown by constant or pulsed voltage/current sources.

• 한국전기전자재료학회논문지
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• 제27권7호
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• pp.433-437
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• 2014

Transparent thin film transistors were fabricated on $n^+$-Si wafers coated by $Al_2O_3/SiO_2$. Zinc tin oxide (ZTO) films deposited by rf magnetron sputtering were employed for active layers. The mobility (${\mu}s$), threshold voltage ($V_T$), and subthreshold swing (SS) dependances on ZTO thickness were analyzed. The $V_T$ decreased with increasing ZTO thickness. The ${\mu}s$ raised from $5.1cm^2/Vsec$ to $27.0cm^2/Vsec$ by increasing ZTO thickness from 7 nm to 12 nm, and then decreased with ZTO thickness above 12 nm. The SS was proportional to ZTO thickness.